Analysis of 13C-NMR spectra in C60 superconductors:: Hyperfine coupling constants, electronic correlation effect, and magnetic penetration depth

被引:20
作者
Sato, N
Tou, H
Maniwa, Y [1 ]
Kikuchi, K
Suzuki, S
Achiba, Y
Kosaka, M
Tanigaki, K
机构
[1] Tokyo Metropolitan Univ, Dept Phys, Hachioji, Tokyo 1920397, Japan
[2] Tokyo Metropolitan Univ, Dept Chem, Hachioji, Tokyo 1920397, Japan
[3] NEC Corp Ltd, Tsukuba, Ibaraki 305, Japan
关键词
D O I
10.1103/PhysRevB.58.12433
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
A C-13-NMR anisotropic hyperfine coupling: tensor was determined as 2 pi(-1.68, -1.68, 3.37) x 10(6) rad/sec for C-60(3-) in A(3)C(60) superconductors, where A is an alkali metal, by analyzing C-13-NMR spectra below 85 K. Combined with an isotropic coupling constant of (2 pi x0.69)x10(6) rad/sec, the 2s and 2p characters of the electronic wave functions at the Fermi level were deduced. The results were compatible with local-density-approximation band calculations. From a simulation of C-13-NMR spectra at superconducting state, the traceless chemical (orbital) shift tensor and isotropic chemical shift were determined as (67, 34, -101) ppm and similar to 150 ppm, respectively. An estimated magnetic penetration depth is larger than 570 nm in K3C60 Furthermore, the modified Korringa relation, T(1)TK(2)similar to beta S (with Knight shift K,: spin-lattice relaxation time T-1, and Korringa constant S), clearly showed the existence of weak but substantial antiferromagnetic spin fluctuation in A(3)C(60); beta=0.40-0.58 with an error of +/-20%. The Stoner enhancement factor was also determined as 1-1.5 from a comparison between spin susceptibility obtained from NMR and band-calculation results. [S0163-1829(98)00542-6].
引用
收藏
页码:12433 / 12440
页数:8
相关论文
共 38 条
[1]   DOMINANCE OF THE SPIN-DIPOLAR NMR RELAXATION MECHANISM IN FULLERENE SUPERCONDUCTORS [J].
ANTROPOV, VP ;
MAZIN, II ;
ANDERSEN, OK ;
LIECHTENSTEIN, AI ;
JEPSEN, O .
PHYSICAL REVIEW B, 1993, 47 (18) :12373-12376
[2]   Mixed-state parameters and vortex pinning in single-crystalline K3C60 fullerene superconductors [J].
Buntar, V ;
Sauerzopf, FM ;
Weber, HW ;
Fischer, JE ;
Kuzmany, H ;
Haluska, M .
PHYSICAL REVIEW B, 1997, 56 (21) :14128-14137
[3]  
Dresselhaus M. S., 1996, SCI FULLERENES CARBO
[4]   P-31-NMR STUDY OF POWDER AND SINGLE-CRYSTAL SAMPLES OF AMMONIUM DIHYDROGEN PHOSPHATE - EFFECT OF HOMONUCLEAR DIPOLAR COUPLING [J].
EICHELE, K ;
WASYLISHEN, RE .
JOURNAL OF PHYSICAL CHEMISTRY, 1994, 98 (12) :3108-3113
[5]   THEORETICAL FERMI-SURFACE PROPERTIES AND SUPERCONDUCTING PARAMETERS FOR K3C60 [J].
ERWIN, SC ;
PICKETT, WE .
SCIENCE, 1991, 254 (5033) :842-845
[6]   ORIENTATIONAL DISORDER AND ELECTRONIC STATES IN C-60 AND A3C60, WHERE A IS AN ALKALI-METAL [J].
GELFAND, MP ;
LU, JP .
PHYSICAL REVIEW LETTERS, 1992, 68 (07) :1050-1053
[7]  
Gennes P. D., 1966, SUPERCONDUCTIVITY ME
[8]   2D NUCLEAR-MAGNETIC-RESONANCE ANALYSIS OF OSMYLATED C60 [J].
HAWKINS, JM ;
LOREN, S ;
MEYER, A ;
NUNLIST, R .
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY, 1991, 113 (20) :7770-7771
[9]   ELECTRONIC-STRUCTURES OF K3C60, RBK2C60, RB2KC60, RB3C60, RB2CSC60, AND CS3C60 CRYSTALS [J].
HUANG, MZ ;
XU, YN ;
CHING, WY .
PHYSICAL REVIEW B, 1992, 46 (10) :6572-6577
[10]   Metal-insulator transition in ammoniated K3C60 [J].
Iwasa, Y ;
Shimoda, H ;
Palstra, TTM ;
Maniwa, Y ;
Zhou, O ;
Mitani, T .
PHYSICAL REVIEW B, 1996, 53 (14) :R8836-R8839